水槽侧壁对任意三维结构波浪力的影响

基于势流理论,采用高阶边界元法在线性频域内研究水槽中波浪对任意结构的作用。探讨水槽侧壁对垂直圆柱和方箱所受到的波浪力的影响,研究水槽宽度与入射波长以及结构特征长度之间的关系,重点研究横向立波的产生及其共振对结构受到的水平力和垂向力的影响。     

三峡电站讯期调峰对两坝间河段通航条件影响的研究

通过模型试验研究,分析三峡电站在泄洪和日调节时产生的非恒定流对两坝间通航条件的影响。     

船模航行试验技术在水运工程研究中的应用

论述了船模航行试验的基本相似条件、相关技术,指出这项技术适于研究航道及通航工程的水流条件及工程方案的优化布置;研究船舶性能、航道尺度、航道水流条件三者的相互关系及提高通航能力的措施。介绍了这项技术在水运工程研究中的应用及发展前景。     

齐岳山隧道F12断层注浆加固技术

注浆技术是通过隧道不良地质的常用方法之一。齐岳山隧道穿越多个断层地段,通过长、中、短超前地质预测预报技术,准确判定隧道围岩地质,施工中采用注浆回固技术通过断层。     

抗拔桩在地下车站主体结构计算模型中的边界条件研究

抗拔桩在地下车站主体结构计算中作为一个边界条件常被设置为3种型式,以广州地铁2、8号线换乘站南洲站的2号线部分作为计算实例,将这3种常见的边界条件进行计算对比分析,提出一个合理的边界条件,可为今后带抗拔桩的地下车站主体结构计算提供参考。     

JT1-CZ型机车信号异常分析

以JT1-CZ型机车为例,通过分析其信号记录器数据,对地面发码设备、机车运行与由机车信号车载设备自身导致的机车信号运行不正常现象提出了一些防范措施,以便提高机车信号车载设备的安全性、可靠性。     

序线性空间中集值优化问题弱有效解的最优性条件

在序线性空间中,引入(u,02;Y )—广义次似凸集值映射,建立了此映射下的一个择一定理.利用此定理,在序线性空间中获得了带广义不等式约束的集值优化问题弱有效解的最优性必要条件和充分条件.     

饱和土与结构动力相互作用影响函数

依据外力作用下两相饱和土介质动力响应的基本解，构造了柱面荷载作用下，饱和土与结构动力相互作用影响函数，解决了用边界元法分析饱和土与结构动力相互作用的关键问题。     

Simple Lagrangian formulation of bubbly flow in a turbulent boundary layer (bubbly boundary layer flow)

For the theoretical consideration of a system for reducing skin friction, a mathematical model was derived to represent, in a two-phase field, the effect on skin friction of the injection of micro air bubbles into the turbulent boundary layer of a liquid stream. Based on the Lagrangian method, the equation of motion governing a single bubble was derived. The random motion of bubbles in a field initially devoid of bubbles was then traced in three dimensions to estimate void fraction distributions across sections of the flow channel, and to determine local bubble behavior. The liquid phase was modeled on the principle of mixing length. Assuming that the force exerted on the liquid phase was equal to the fluid drag generated by bubble slip, an equation was derived to express the reduction in turbulent shear stress. Corroborating experimental data were obtained from tests using a cavitation tunnel equipped with a slit in the ceiling from which bubbly water was injected. The measurement data provided qualitative substantiation of the trend shown by the calculated results with regard to the skin friction ratio between cases with and without bubble injection as function of the distance downstream from the point of bubble injection.List of symbols B law of wall constant - C _f local coefficient of skin friction - C _f0 local coefficient of skin friction in the absence of bubbles - d _b bubble diameter [m] - g acceleration of gravity [m/s²] - k ₁ k₄ proportional coefficient - k _L turbulent energy of the liquid phase [m²/s²] - L representative length [m] - l _b mean free path of a bubble [m] - m _A added mass of a single bubble [kg] - m _b mass of a single bubble [kg] - N _x ,N _y ,N _z force perpendicular to the wall or ceiling exerted on a bubble adhering to that wall or ceiling [N] - P absolute pressure [Pa] - Q _G rate of air supply [/min] - q _L ⁽ⁱ⁾ turbulent velocity at the ith time increment [m/s] - R> _ex Reynolds number defined by Eq. 32 - T _*L integral time scale of the liquid phase [s] - U velocity of the main stream [m/s] - ,¯v,¯w time-averaged velocity components [m/s] - u,v,w turbulent velocity components [m/s] - û _L ,v_L root mean square values of liquid phase turbulence components in thex- and y-directions [m/s] - V volume of a single bubble [m³] - X,Y,Z components of bubble displacement [m] - x _s ,y _s ,z _s coordinate of a random point on a sphere of unit diameter centered at the coordinate origin - root mean square of bubble displacement in they-direction in reference to the turbulent liquid phase velocity [m] - local void fraction - _m mean void fraction in a turbulent region - regular random number - R _v increment of the horizontal component of the force acting on a single bubble, defined by Eq. 22 [N] - t time increment [s] - ₁ reduction of turbulent stress [N/m²] - _L rate of liquid energy dissipation [m²/s³] - _m coefficient defined by Eq. 30 - law of wall constant in the turbulent region in absence of bubbles - ₁ law of wall constant in the turbulent region in presence of bubbles     

水下砂卵石地层盾构隧道越江段注浆压力研究

近年来,江(海)底盾构隧道建设日益增多,对于水下段而言,由于地层渗透性强、埋深浅等因素影响,盾尾同步注浆压力的合理控制显得尤其重要,而探明盾构隧道在施工过程中孔隙水压力的分布对工程实践意义重大。本文依托常德沅江过江隧道工程,结合工程现场地形、地质、气候以及水文条件,采用FLAC^3D有限元分析软件对盾构施工扰动下的地层孔隙水压力分布进行系统分析。研究结果表明:(1)综合考虑各种因素确定渗流场中削减边界为20 m,即模型构建时沿开挖方向前后多取20 m长度,可使模拟结果更能真实反映越江隧道围岩各处孔隙水压力的变化规律;(2)盾构隧道掘进过程中,拱顶、拱底和左右拱腰处的动水压随掘进距离的变化趋势大致相同,拱底动水压量值最大,左右拱腰次之,拱顶最小,并根据区间动水压力变化规律给出满足岸边段和水下段要求的注浆压力。